TY - JOUR
T1 - Holographic technicolor models and their S-parameter
AU - Mintakevich, Oded
AU - Sonnenschein, Jacob
PY - 2009
Y1 - 2009
N2 - We study the Peskin-Takeuchi S-parameter of holographic technicolor models. We present the recipe for computing the parameter in a generalized holographic setup. We then apply it to several holographic models that include: (a) the Sakai-Sugimoto model and (b) its non-compactified cousin, (c) a non-critical analog of (a) based on near extremal AdS 6 background, (d) the KMMW model which is similar to model (a) but with D6 and anti-D6 flavor branes replacing the D8 and anti-D8 branes, (e) a model based on D5 branes compactified on two S 1s with D7 and anti-D7 probe branes and (f) the conifold model with the same probe branes as in (e). The models are gravity duals of gauge theories with SU(N TC) gauge theory and with a breakdown of a flavor symmetry U(N TF) × U(N TF) U V(N TF). The models (a), (c),(d) and (e) are duals of a confining gauge theories whereas (b) and (f) associate with non confining models. The S-parameter was found to be S=sN TC where s is given by 0.017λ TC, 0.016λ TC, 0.095, 0.50 and 0.043 for the (a), (b), (c), (d), (f) models respectively and for model (e) s is divergent. These results are valid in the large N TC and large λ TC limit. We further derive the dependence of the S-parameter on the ''string endpoint" mass of the techniquarks for the various models. We compute the masses of the low lying vector technimesons.
AB - We study the Peskin-Takeuchi S-parameter of holographic technicolor models. We present the recipe for computing the parameter in a generalized holographic setup. We then apply it to several holographic models that include: (a) the Sakai-Sugimoto model and (b) its non-compactified cousin, (c) a non-critical analog of (a) based on near extremal AdS 6 background, (d) the KMMW model which is similar to model (a) but with D6 and anti-D6 flavor branes replacing the D8 and anti-D8 branes, (e) a model based on D5 branes compactified on two S 1s with D7 and anti-D7 probe branes and (f) the conifold model with the same probe branes as in (e). The models are gravity duals of gauge theories with SU(N TC) gauge theory and with a breakdown of a flavor symmetry U(N TF) × U(N TF) U V(N TF). The models (a), (c),(d) and (e) are duals of a confining gauge theories whereas (b) and (f) associate with non confining models. The S-parameter was found to be S=sN TC where s is given by 0.017λ TC, 0.016λ TC, 0.095, 0.50 and 0.043 for the (a), (b), (c), (d), (f) models respectively and for model (e) s is divergent. These results are valid in the large N TC and large λ TC limit. We further derive the dependence of the S-parameter on the ''string endpoint" mass of the techniquarks for the various models. We compute the masses of the low lying vector technimesons.
KW - AdS-CFT Correspondence
KW - Compactification and String Models
KW - Gauge-gravity correspondence
KW - Technicolor and Composite Models
UR - http://www.scopus.com/inward/record.url?scp=70350033491&partnerID=8YFLogxK
U2 - 10.1088/1126-6708/2009/07/032
DO - 10.1088/1126-6708/2009/07/032
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AN - SCOPUS:70350033491
VL - 2009
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
SN - 1126-6708
IS - 7
M1 - 032
ER -